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2 The lines of longitude are an excellent example of the failure of Euclid's axiom; as they cross the equator they are all parallel to one another but rather than remaining a constant distance apart they meet at both poles If we draw a triangle on a sphere, we find that the angles do not add up to 1800 degrees either The easiest example to think about is to start at the North Pole Draw two straight lines down to the equator, ninety degrees apart, and then join them with a line on the equator You have drawn a triangle in which all three angles are 90 0 , shown in Figure 41 The circumference of a circle also fails to obey the normal law Suppose we draw a circle at a radius r from the North Pole, and we'll choose r so that our circle is the equator.



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Here the most rapidly varying quantity is n, the number of interfering beams But we cannot set a low value for it because the very purpose of a multiple-beam Fizeau is to produce high-quality, high- nesse fringes that require superposition of a large number of regularly delayed beams; this number, in turn, depends on the re ectance of the surfaces The broken curve in Figure 64 shows how the nesse NR (the ratio of the fringe interval to the full width of a fringe at half the height from its peak) of Fabry Perot fringes increases with increasing re ectance The solid curve in the same gure shows the effective number of beams M added by a computer to obtain a peak transmittance within 01 % of the ideal Airy value [in nite sum of Eq (61)] for different re ectances.





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That radius, measured on the surface of the sphere, corresponds to a quarter of a complete circle around the Earth, so r = 1r R/2 where R is the radius of the Earth However, the circumference c is given by 21r R, so instead of the usual relation one has c = 4r for a circle drawn at the equator The circumference is less than 21rr Problem 41 looks at the general case; you may find it helpful to glance at the figure on page 31 now Although I have only considered specific cases where the algebra is easy it is true that whatever triangle or circle is drawn, you'll always find The angles of a triangle add up to more than 1800 The circumference of a circle is less than 21rr..

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It can be seen that for a re ectance below 90%, the effective number of beams M that are superposed to obtain a nesse NR is roughly equal to 2NR For higher re ectivity, the required value of M steadily increases See also Eq (65) and the rationale given there These curves can be exploited for Fizeau interferometry in the following manner p If the surfaces to be tested have a given re ectance R (or equivalently, R R1 R2 when the re ectances are different for the surfaces), or one requires a desired nesse NR such that the re ectance is R, then the curves of Figure 64 indicate the value of M, the effective number of beams that are superposed Then to maintain the Tolansky inequality, one substitutes M for n in Eq (69) and reduces the values of E and t accordingly.

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Tolansky (1948a) gave some typical values of n; E, and t for obtaining symmetric Fizeau fringes The lowest limit of t, the plate separation, is usually.

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